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BSM fits for rare B decays
- Source :
- PoS, 17th International Conference on B-Physics at Frontier Machines, 17th International Conference on B-Physics at Frontier Machines, May 2018, La Biodola, Italy. pp.040, ⟨10.22323/1.326.0040⟩
- Publication Year :
- 2018
- Publisher :
- HAL CCSD, 2018.
-
Abstract
- International audience; The LHCb experiment has made several measurements in $b \to s$ transitions which indicate tensions with the Standard Model predictions.We examine how the significance of the tensions in $B \to K^* \mu^+\mu^-$ observables depend on the various theory implementations of the long-distance effects.We also consider a general parameterisation, consistent with the analyticity structure of the amplitudes and make a statistical comparison to find whether the most favoured explanation of the anomalies is new physics or underestimated hadronic effects.Furthermore, assuming the source of the anomalies to be new physics, to get a fair view of how significantly favoured it is, we perform a global fit to all the Wilson coefficients which can effectively receive beyond the Standard Model contributions.
- Subjects :
- Physics
operator: Wilson
Particle physics
B: semileptonic decay
new physics
effective Hamiltonian
Physics beyond the Standard Model
Hadron
operator: scalar
Structure (category theory)
Observable
LHC-B
Standard Model
analytic properties
Amplitude
statistical analysis
[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]
[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]
effect: hadronic
operator: pseudoscalar
B: branching ratio
numerical calculations
Particle Physics - Experiment
B: rare decay
Particle Physics - Phenomenology
Subjects
Details
- Language :
- English
- Database :
- OpenAIRE
- Journal :
- PoS, 17th International Conference on B-Physics at Frontier Machines, 17th International Conference on B-Physics at Frontier Machines, May 2018, La Biodola, Italy. pp.040, ⟨10.22323/1.326.0040⟩
- Accession number :
- edsair.doi.dedup.....dec5d7f202b47cc6f26e42e8d0fd0f8c